Large Hadron Collider

Size: px
Start display at page:

Download "Large Hadron Collider"

Transcription

1 Large Hadron Collider Himadri Barman TSU, JNCASR September 18,

2 Large Hadron Collider (LHC): Plan We ll see 4 short videos. In between I ll give you a little guideline. Purpose is to understand the event at very basic level. After we finish the last video, we ll have an open discussion. So no questions in between (Time-management courtesy ). 1

3 What s LHC? What happens inside LHC? Proton accelerator of the energy 7 TeV two proton beams are being sent in opposite direction to collide each other. Contained in a circular tunnel circumference = 27 kilometres (17 mi) depth from 50 to 175 metres underground. 2

4 LHC design 3

5 ATLAS: A Toroidal LHC Apparatus. CMS: Compact Muon Solenoid. LHCb: LHC-beauty. ALICE: A Large Ion Collider Experiment. TOTEM: Total Cross Section, Elastic Scattering and Diffraction Dissociation. LHCf: LHC-forward. LHC: preaccelerators. p and Pb: Linear accelerators for protons (Linac 2) and Lead (Linac 3). (not marked) Proton Synchrotron Booster. PS: Proton Synchrotron. SPS: Super Proton Synchrotron. 4

6 VIDEO-1 5

7 We are talking about TeV 1 TeV =10 12 ev Energy scale An adult female mosquito weighs only about 2.0 milligrams 1 ev = 1.6 x Joules 1 TeV = 1.6 x x Joules = 1.6 x 10 7 Joules 1/2 m v 2 = 1.6 x 10 7 Joules, m = 2 x 10 6 kg therefore v = 0.4 m/s = 1.4 kph Apparently Mosquitoes can fly about 1 to 1.5 miles per hour. 1 mph = 1.6 kph so our mosquito is a little slow, but the comparison is a good one. (Courtesy: glossary.htm) 6

8 Hopes for outcoming physics 1. Higgs Boson (Standard Model): 2. SUSY (Beyond standard model): 3. Extra dimension (String Thoery): 7

9 Higgs Boson First let s look at the Standard Model (Murray Gell-Mann 69) 2 classes of particles: A. Matter building particles: Fermions (half-integral spins) 6 Quarks: u,d;c,s;t,b and their anti-particles 6 Leptons: e,ν e ;µ,ν µ ;τ,ν τ and their anti-particles B. Force mediating particles: Bosons (integral spins) 4 fundamental forces exists in nature! Electromagnetic force is mediated by photons (γ) [eg. Coulomb force, magnetic force, EM force]. Weak force is mediated by W ± and Z bosons [eg. β-decay]. Strong force is mediated by gluons (g) [eg. Force to hold protons and 8

10 neutron together in a nucleus]. Gravitational force is mediated by gravitons (yet not found and not in SM) [eg. Force that makes an apple fall down]. Now what are hadrons? Particles made up of quarks and held together by strong forces. Best known examples : protons (p) and neutrons (n). 9

11 VIDEO-2 and VIDEO-3 10

12 But where are the Higgs? Goldstone s Theorem: For every spontaneously broken continuous symmetry, there must exist a massless boson (J. Goldstone, 1961). E+W unification Electroweak (EW) force: (Abdus Salam, Sheldon Glashow and Steven Weinberg ( 68), Nobel Prize 79) Used Non-Abelian gauge theory (Yang-Mills) with gauge bosons such as W and Z particles. But gauge bosons should be massless! Break the symmetry. Spontaneous symmetry breaking (SSB). 11

13 One massless vector boson (photon)+two massive vector bosons (W and Z) + one scalar boson (Higgs particle?) found. Wait! Goldstone s theorem (GT) says, SSB means existence of massless bosons. Then...? Ans. SSB+gauge theory overrules GT. This is the Higgs theory (Higgs 64)! Since other mediators are also gauge bosons, it s assumed that they also becomes massive due to the Higgs field Higgs is responsible for matters to have masses So don t we see Higgs at all? Yes! In cond. matt physics. Superconductor! Photons get mass in relativistic sense (Meissner effect) (Anderson 63) 12

14 Supersymmetry (SUSY), beyond standard model Motivation: Hierarchy problem problem with Higgs mass. For every type of boson there exists a corresponding type of fermion, and vice-versa. Supersymmetry partners are called sparticles eg. electron has selectron (spin 0), photon has photino (spin 1/2), Higgs (spin 0) has Higgsino (spin 1/2). sparticle may have higher mass compared to their particle-partner. WIMP (Weakly interacting massive particles) are supposed be candidates for Dark Matter 13

15 Extra dimension, string theory Black holes are produced at the energy scale of the order of Plank scale (Planck mass= 1.22 X GeV/c 2 ). It can form at weak scale too! String theory is there to help. (Randall-Sundrum model, ADD model : 4 spatial dimensions). Black hole!!! Earth will be swallowed!!!??? No! Hawking radiation is there BH s are tiny Radiation will be higher and faster evaporate as soon as they form. Now Hawking has a chance to get a Nobel Prize! 14

16 VIDEO-4: TED Talk by Dr. Brian Cox 15

17 Questions Why TeV? What s SSB? 16

An Introduction to Particle Physics

An Introduction to Particle Physics An Introduction to Particle Physics The Universe started with a Big Bang The Universe started with a Big Bang What is our Universe made of? Particle physics aims to understand Elementary (fundamental)

More information

The God particle at last? Astronomy Ireland, Oct 8 th, 2012

The God particle at last? Astronomy Ireland, Oct 8 th, 2012 The God particle at last? Astronomy Ireland, Oct 8 th, 2012 Cormac O Raifeartaigh Waterford Institute of Technology CERN July 4 th 2012 (ATLAS and CMS ) A new particle of mass 125 GeV I The Higgs boson

More information

Physics Beyond the Standard Model. Marina Cobal Fisica Sperimentale Nucleare e Sub-Nucleare

Physics Beyond the Standard Model. Marina Cobal Fisica Sperimentale Nucleare e Sub-Nucleare Physics Beyond the Standard Model Marina Cobal Fisica Sperimentale Nucleare e Sub-Nucleare Increasingly General Theories Grand Unified Theories of electroweak and strong interactions Supersymmetry

More information

Fundamental Particles and Forces

Fundamental Particles and Forces Fundamental Particles and Forces A Look at the Standard Model and Interesting Theories André Gras PHYS 3305 SMU 1 Overview Introduction to Fundamental Particles and Forces Brief History of Discovery The

More information

Beyond the standard model? From last time. What does the SM say? Grand Unified Theories. Unifications: now and the future

Beyond the standard model? From last time. What does the SM say? Grand Unified Theories. Unifications: now and the future From last time Quantum field theory is a relativistic quantum theory of fields and interactions. Fermions make up matter, and bosons mediate the forces by particle exchange. Lots of particles, lots of

More information

First some Introductory Stuff => On The Web.

First some Introductory Stuff => On The Web. First some Introductory Stuff => On The Web http://hep.physics.utoronto.ca/~orr/wwwroot/phy357/phy357s.htm PHY357 = What is the Universe Made Of? Is the Universe Made of These? Proton = (u u d) held

More information

A first trip to the world of particle physics

A first trip to the world of particle physics A first trip to the world of particle physics Itinerary Massimo Passera Padova - 13/03/2013 1 Massimo Passera Padova - 13/03/2013 2 The 4 fundamental interactions! Electromagnetic! Weak! Strong! Gravitational

More information

The Discovery of the Higgs Boson: one step closer to understanding the beginning of the Universe

The Discovery of the Higgs Boson: one step closer to understanding the beginning of the Universe The Discovery of the Higgs Boson: one step closer to understanding the beginning of the Universe Anna Goussiou Department of Physics, UW & ATLAS Collaboration, CERN Kane Hall, University of Washington

More information

FACULTY OF SCIENCE. High Energy Physics. WINTHROP PROFESSOR IAN MCARTHUR and ADJUNCT/PROFESSOR JACKIE DAVIDSON

FACULTY OF SCIENCE. High Energy Physics. WINTHROP PROFESSOR IAN MCARTHUR and ADJUNCT/PROFESSOR JACKIE DAVIDSON FACULTY OF SCIENCE High Energy Physics WINTHROP PROFESSOR IAN MCARTHUR and ADJUNCT/PROFESSOR JACKIE DAVIDSON AIM: To explore nature on the smallest length scales we can achieve Current status (10-20 m)

More information

BACKGROUND LHC Physics Program Summary LHC PHYSICS. Andrés G. Delannoy 1. 1 Vanderbilt University. 2014/07/21 1

BACKGROUND LHC Physics Program Summary LHC PHYSICS. Andrés G. Delannoy 1. 1 Vanderbilt University. 2014/07/21 1 2014/07/21 delannoy@cern.ch 1 LHC PHYSICS Andrés G. Delannoy 1 1 Vanderbilt University 2014/07/21 delannoy@cern.ch 2 1 BACKGROUND The Large Hadron Collider The Standard Model The Higgs Mechanism SuperSymmetry

More information

The Why, What, and How? of the Higgs Boson

The Why, What, and How? of the Higgs Boson Modern Physics The Why, What, and How? of the Higgs Boson Sean Yeager University of Portland 10 April 2015 Outline Review of the Standard Model Review of Symmetries Symmetries in the Standard Model The

More information

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions.

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Overview The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Our understanding is about to take a giant leap.. the Large Hadron Collider

More information

The God particle at last? Science Week, Nov 15 th, 2012

The God particle at last? Science Week, Nov 15 th, 2012 The God particle at last? Science Week, Nov 15 th, 2012 Cormac O Raifeartaigh Waterford Institute of Technology CERN July 4 th 2012 (ATLAS and CMS ) A new particle of mass 125 GeV Why is the Higgs particle

More information

Lecture 39, 40 Supplement: Particle physics in the LHC era

Lecture 39, 40 Supplement: Particle physics in the LHC era Lecture 39, 40 Supplement: Particle physics in the LHC era The Matter Particles (Fermions) plus their antiparticles... What is measured? quarks confined into hadrons A zoo of strongly interacting particles...

More information

Particle + Physics at ATLAS and the Large Hadron Coillder

Particle + Physics at ATLAS and the Large Hadron Coillder Particle + Physics at ATLAS and the Large Hadron Coillder Discovering the elementary particles of the Universe Kate Shaw The International Centre for Theoretical Physics + Overview Introduction to Particle

More information

I. Antoniadis CERN. IAS CERN Novice Workshop, NTU, 7 Feb 2014

I. Antoniadis CERN. IAS CERN Novice Workshop, NTU, 7 Feb 2014 I. Antoniadis CERN IAS CERN Novice Workshop, NTU, 7 Feb 2014 1 2 3 the Large Hadron Collider (LHC) Largest scientific instrument ever built, 27km of circumference >10 000 people involved in its design

More information

Physics 4213/5213 Lecture 1

Physics 4213/5213 Lecture 1 August 28, 2002 1 INTRODUCTION 1 Introduction Physics 4213/5213 Lecture 1 There are four known forces: gravity, electricity and magnetism (E&M), the weak force, and the strong force. Each is responsible

More information

Most of Modern Physics today is concerned with the extremes of matter:

Most of Modern Physics today is concerned with the extremes of matter: Most of Modern Physics today is concerned with the extremes of matter: Very low temperatures, very large numbers of particles, complex systems Æ Condensed Matter Physics Very high temperatures, very large

More information

Analyzing CMS events

Analyzing CMS events Quarknet University of Rochester, March 23, 2012 Analyzing CMS events Questions in Particle Physics Introducing the Standard Model The Large Hadron Collider The CMS detector W and Z bosons: decays ispy

More information

Most of Modern Physics today is concerned with the extremes of matter:

Most of Modern Physics today is concerned with the extremes of matter: Most of Modern Physics today is concerned with the extremes of matter: Very low temperatures, very large numbers of particles, complex systems Æ Condensed Matter Physics Very high temperatures, very large

More information

Kiwoon Choi (KAIST) 3 rd GCOE Symposium Feb (Tohoku Univ.)

Kiwoon Choi (KAIST) 3 rd GCOE Symposium Feb (Tohoku Univ.) Exploring New Physics beyond the Standard Model of Particle Physics Kiwoon Choi (KAIST) 3 rd GCOE Symposium Feb. 2011 (Tohoku Univ.) We are confronting a critical moment of particle physics with the CERN

More information

The mass of the Higgs boson

The mass of the Higgs boson The mass of the Higgs boson LHC : Higgs particle observation CMS 2011/12 ATLAS 2011/12 a prediction Higgs boson found standard model Higgs boson T.Plehn, M.Rauch Spontaneous symmetry breaking confirmed

More information

Weak interactions and vector bosons

Weak interactions and vector bosons Weak interactions and vector bosons What do we know now about weak interactions? Theory of weak interactions Fermi's theory of weak interactions V-A theory Current - current theory, current algebra W and

More information

Origin of the Universe - 2 ASTR 2120 Sarazin. What does it all mean?

Origin of the Universe - 2 ASTR 2120 Sarazin. What does it all mean? Origin of the Universe - 2 ASTR 2120 Sarazin What does it all mean? Fundamental Questions in Cosmology 1. Why did the Big Bang occur? 2. Why is the Universe old? 3. Why is the Universe made of matter?

More information

PHY323:Lecture 11 SUSY and UED Higgs and Supersymmetry The Neutralino Extra Dimensions How WIMPs interact

PHY323:Lecture 11 SUSY and UED Higgs and Supersymmetry The Neutralino Extra Dimensions How WIMPs interact PHY323:Lecture 11 SUSY and UED Higgs and Supersymmetry The Neutralino Extra Dimensions How WIMPs interact Candidates for Dark Matter III The New Particle Zoo Here are a few of the candidates on a plot

More information

The Discovery of the Higgs boson Matthew Herndon, University of Wisconsin Madison Physics 301: Physics Today. M. Herndon, Phys

The Discovery of the Higgs boson Matthew Herndon, University of Wisconsin Madison Physics 301: Physics Today. M. Herndon, Phys The Discovery of the Higgs boson Matthew Herndon, University of Wisconsin Madison Physics 301: Physics Today M. Herndon, Phys 301 2018 1 The Periodic Table: The early 20 th century understanding of the

More information

Where are we heading? Nathan Seiberg IAS 2014

Where are we heading? Nathan Seiberg IAS 2014 Where are we heading? Nathan Seiberg IAS 2014 Purpose of this talk A brief, broad brush status report of particle physics Where we are How we got here (some historical perspective) Problems and challenges

More information

Lecture 18 - Beyond the Standard Model

Lecture 18 - Beyond the Standard Model Lecture 18 - Beyond the Standard Model Why is the Standard Model incomplete? Grand Unification Baryon and Lepton Number Violation More Higgs Bosons? Supersymmetry (SUSY) Experimental signatures for SUSY

More information

Particle Physics. Tommy Ohlsson. Theoretical Particle Physics, Department of Physics, KTH Royal Institute of Technology, Stockholm, Sweden

Particle Physics. Tommy Ohlsson. Theoretical Particle Physics, Department of Physics, KTH Royal Institute of Technology, Stockholm, Sweden Particle Physics Tommy Ohlsson Theoretical Particle Physics, Department of Physics, KTH Royal Institute of Technology, Stockholm, Sweden International Baccalaureate T. Ohlsson (KTH) Particle Physics 1/

More information

Lecture 03. The Standard Model of Particle Physics. Part II The Higgs Boson Properties of the SM

Lecture 03. The Standard Model of Particle Physics. Part II The Higgs Boson Properties of the SM Lecture 03 The Standard Model of Particle Physics Part II The Higgs Boson Properties of the SM The Standard Model So far we talked about all the particles except the Higgs If we know what the particles

More information

Discovery Physics at the Large Hadron Collider

Discovery Physics at the Large Hadron Collider + / 2 GeV N evt 4 10 3 10 2 10 CMS 2010 Preliminary s=7 TeV -1 L dt = 35 pb R > 0.15 R > 0.20 R > 0.25 R > 0.30 R > 0.35 R > 0.40 R > 0.45 R > 0.50 10 1 100 150 200 250 300 350 400 [GeV] M R Discovery

More information

Astronomy 182: Origin and Evolution of the Universe

Astronomy 182: Origin and Evolution of the Universe Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 12 Nov. 18, 2015 Today Big Bang Nucleosynthesis and Neutrinos Particle Physics & the Early Universe Standard Model of Particle

More information

Electroweak Symmetry Breaking

Electroweak Symmetry Breaking Electroweak Symmetry Breaking An enduring mystery of the standard model of particle physics and how we hope to solve it David Schaich Department of Physics and Center for Computational Science Boston University

More information

The Standard Model and Beyond

The Standard Model and Beyond The Standard Model and Beyond Nobuchika Okada Department of Physics and Astronomy The University of Alabama 2011 BCVSPIN ADVANCED STUDY INSTITUTE IN PARTICLE PHYSICS AND COSMOLOGY Huê, Vietnam, 25-30,

More information

November 24, Scalar Dark Matter from Grand Unified Theories. T. Daniel Brennan. Standard Model. Dark Matter. GUTs. Babu- Mohapatra Model

November 24, Scalar Dark Matter from Grand Unified Theories. T. Daniel Brennan. Standard Model. Dark Matter. GUTs. Babu- Mohapatra Model Scalar from November 24, 2014 1 2 3 4 5 What is the? Gauge theory that explains strong weak, and electromagnetic forces SU(3) C SU(2) W U(1) Y Each generation (3) has 2 quark flavors (each comes in one

More information

The ATLAS Experiment and the CERN Large Hadron Collider

The ATLAS Experiment and the CERN Large Hadron Collider The ATLAS Experiment and the CERN Large Hadron Collider HEP101-2 January 28, 2013 Al Goshaw 1 HEP 101-2 plan Jan. 14: Introduction to CERN and ATLAS DONE Today: 1. Comments on grant opportunities 2. Overview

More information

SUPERSYMETRY FOR ASTROPHYSICISTS

SUPERSYMETRY FOR ASTROPHYSICISTS Dark Matter: From the Cosmos to the Laboratory SUPERSYMETRY FOR ASTROPHYSICISTS Jonathan Feng University of California, Irvine 29 Jul 1 Aug 2007 SLAC Summer Institute 30 Jul 1 Aug 07 Feng 1 Graphic: N.

More information

Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material. From last time

Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material. From last time Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material From last time Quantum field theory is a relativistic quantum theory of fields and interactions. Fermions

More information

Theoretical High Energy Physics in the LHC Era

Theoretical High Energy Physics in the LHC Era Theoretical High Energy Physics in the LHC Era Talk to Physics 205, Jan. 2013 Department of Physics and Santa Cruz Institute for Particle Physics University of California, Santa Cruz January, 2013 We have

More information

XI. Beyond the Standard Model

XI. Beyond the Standard Model XI. Beyond the Standard Model While the Standard Model appears to be confirmed in all ways, there are some unclear points and possible extensions: Why do the observed quarks and leptons have the masses

More information

MINERVA Masterclass. Teachers Manual. Vera Zimanyine Horvath Francesco Mezzanotte Tom Lambert

MINERVA Masterclass. Teachers Manual. Vera Zimanyine Horvath Francesco Mezzanotte Tom Lambert MINERVA Masterclass Teachers Manual Vera Zimanyine Horvath Francesco Mezzanotte Tom Lambert 1 Fundamental Particles theoretical background of using Minerva for teachers 1. Standard Model of Fundamental

More information

Physics 662. Particle Physics Phenomenology. February 21, Physics 662, lecture 13 1

Physics 662. Particle Physics Phenomenology. February 21, Physics 662, lecture 13 1 Physics 662 Particle Physics Phenomenology February 21, 2002 Physics 662, lecture 13 1 Physics Beyond the Standard Model Supersymmetry Grand Unified Theories: the SU(5) GUT Unification energy and weak

More information

String Theory in the LHC Era

String Theory in the LHC Era String Theory in the LHC Era J Marsano (marsano@uchicago.edu) 1 String Theory in the LHC Era 1. Electromagnetism and Special Relativity 2. The Quantum World 3. Why do we need the Higgs? 4. The Standard

More information

Search for SUperSYmmetry SUSY

Search for SUperSYmmetry SUSY PART 3 Search for SUperSYmmetry SUSY SUPERSYMMETRY Symmetry between fermions (matter) and bosons (forces) for each particle p with spin s, there exists a SUSY partner p~ with spin s-1/2. q ~ g (s=1)

More information

Supersymmetry and how it helps us understand our world

Supersymmetry and how it helps us understand our world Supersymmetry and how it helps us understand our world Spitalfields Day Gauge Theory, String Theory and Unification, 8 October 2007 Theoretical Physics Institute, University of Minnesota What is supersymmetry?

More information

Lecture PowerPoint. Chapter 32 Physics: Principles with Applications, 6 th edition Giancoli

Lecture PowerPoint. Chapter 32 Physics: Principles with Applications, 6 th edition Giancoli Lecture PowerPoint Chapter 32 Physics: Principles with Applications, 6 th edition Giancoli 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the

More information

Phenomenology of Heavy-Ion Collisions

Phenomenology of Heavy-Ion Collisions Phenomenology of Heavy-Ion Collisions Hendrik van Hees Goethe University Frankfurt and FIAS October 2, 2013 Hendrik van Hees (GU Frankfurt/FIAS) HIC Phenomenology October 2, 2013 1 / 20 Outline 1 Plan

More information

Electroweak Physics at the LHC Introductory Lecture

Electroweak Physics at the LHC Introductory Lecture Electroweak Physics at the LHC Introductory Lecture Stefan Dittmaier MPI München Universität Wien, October 2007 Stefan Dittmaier (MPI München), Electroweak Physics at the LHC Introductory Lecture 1 1 The

More information

Where are we heading? Nathan Seiberg IAS 2016

Where are we heading? Nathan Seiberg IAS 2016 Where are we heading? Nathan Seiberg IAS 2016 Two half-talks A brief, broad brush status report of particle physics and what the future could be like The role of symmetries in physics and how it is changing

More information

Elementary particles and typical scales in high energy physics

Elementary particles and typical scales in high energy physics Elementary particles and typical scales in high energy physics George Jorjadze Free University of Tbilisi Zielona Gora - 23.01.2017 GJ Elementary particles and typical scales in HEP Lecture 1 1/18 Contents

More information

The Early Universe. Overview: The Early Universe. Accelerators recreate the early universe. Simple Friedmann equation for the radiation era:

The Early Universe. Overview: The Early Universe. Accelerators recreate the early universe. Simple Friedmann equation for the radiation era: The Early Universe Notes based on Teaching Company lectures, and associated undergraduate text with some additional material added. ) From µs to s: quark confinement; particle freezout. 2) From s to 3

More information

Lecture 03. The Standard Model of Particle Physics. Part III Extensions of the Standard Model

Lecture 03. The Standard Model of Particle Physics. Part III Extensions of the Standard Model Lecture 03 The Standard Model of Particle Physics Part III Extensions of the Standard Model Where the SM Works Excellent description of 3 of the 4 fundamental forces Explains nuclear structure, quark confinement,

More information

Introduction to Elementary Particle Physics. Note 01 Page 1 of 8. Natural Units

Introduction to Elementary Particle Physics. Note 01 Page 1 of 8. Natural Units Introduction to Elementary Particle Physics. Note 01 Page 1 of 8 Natural Units There are 4 primary SI units: three kinematical (meter, second, kilogram) and one electrical (Ampere 1 ) It is common in the

More information

Unravelling the Mysteries of Matter with the CERN Large Hadron Collider An Introduction/Overview of Particle Physics

Unravelling the Mysteries of Matter with the CERN Large Hadron Collider An Introduction/Overview of Particle Physics Unravelling the Mysteries of Matter with the CERN Large Hadron Collider An Introduction/Overview of Particle Physics Introductory Lecture August 3rd 2014 International Centre for Theoretical Physics and

More information

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS Class Mechanics My office (for now): Dantziger B Room 121 My Phone: x85200 Office hours: Call ahead, or better yet, email... Even better than office

More information

Introduction to the Standard Model

Introduction to the Standard Model Introduction to the Standard Model Bill Murray, RAL, Quarks and leptons Bosons and forces The Higgs March 2002 1 Outline: An introduction to particle physics What is the Higgs Boson? Some unanswered questions

More information

Introduction to Particle Physics. HST July 2016 Luis Alvarez Gaume 1

Introduction to Particle Physics. HST July 2016 Luis Alvarez Gaume 1 Introduction to Particle Physics HST July 2016 Luis Alvarez Gaume 1 Basics Particle Physics describes the basic constituents of matter and their interactions It has a deep interplay with cosmology Modern

More information

Kaluza-Klein Dark Matter

Kaluza-Klein Dark Matter Kaluza-Klein Dark Matter Hsin-Chia Cheng UC Davis Pre-SUSY06 Workshop Complementary between Dark Matter Searches and Collider Experiments Introduction Dark matter is the best evidence for physics beyond

More information

Bosons in the Zoo of Elementary Particles

Bosons in the Zoo of Elementary Particles Bosons in the Zoo of Elementary Particles Daniele Sasso * Abstract In this paper we want to raise the question concerning the physical identity of bosons and the function that they perform in the Non-Standard

More information

The Higgs discovery - a portal to new physics

The Higgs discovery - a portal to new physics The Higgs discovery - a portal to new physics Department of astronomy and theoretical physics, 2012-10-17 1 / 1 The Higgs discovery 2 / 1 July 4th 2012 - a historic day in many ways... 3 / 1 July 4th 2012

More information

Mysteries of the Standard Model

Mysteries of the Standard Model Mysteries of the Standard Model Methods of exploring the nature of the Electroweak force at the Compact Muon Solenoid [CMS] experiment. Final REU presentation given by Kellen McGee in partial fulfillment

More information

High Energy Physics. QuarkNet summer workshop June 24-28, 2013

High Energy Physics. QuarkNet summer workshop June 24-28, 2013 High Energy Physics QuarkNet summer workshop June 24-28, 2013 1 The Birth of Particle Physics In 1896, Thompson showed that electrons were particles, not a fluid. In 1905, Einstein argued that photons

More information

Quanta to Quarks. Science Teachers Workshop 2014 Workshop Session. Adrian Manning

Quanta to Quarks. Science Teachers Workshop 2014 Workshop Session. Adrian Manning Quanta to Quarks Science Teachers Workshop 2014 Workshop Session Adrian Manning The Quanta to Quarks module! The Quanta to Quarks module ultimately deals with some of the most fundamental questions about

More information

The discovery of W ± and Z 0 vector-bosons

The discovery of W ± and Z 0 vector-bosons The discovery of W ± and Z 0 vector-bosons Giulia De Zordo April 15, 2014 Abstract This article is about the discovery of the W ± and Z 0 vector-bosons, the carriers of weak interaction. The discovery

More information

What is the HIGGS BOSON and why does physics need it?

What is the HIGGS BOSON and why does physics need it? What is the HIGGS BOSON and why does physics need it? Stephen Naculich, Department of Physics Uncommon Hour Talk, May 3, 2013 THE HIGGS BOSON 1964: new particle predicted by Peter Higgs THE HIGGS BOSON

More information

Modern physics 1 Chapter 13

Modern physics 1 Chapter 13 Modern physics 1 Chapter 13 13. Particle physics Particle studied within the ATLAS-project CERN In the beginning of 1930, it seemed that all the physics fundaments was placed within the new areas of elementary

More information

Where are we heading?

Where are we heading? Where are we heading? PiTP 2013 Nathan Seiberg IAS Purpose of this talk A brief, broad brush status report of particle physics Where we are How we got here (some historical perspective) What are the problems

More information

Wesley Smith, U. Wisconsin, January 21, Physics 301: Introduction - 1

Wesley Smith, U. Wisconsin, January 21, Physics 301: Introduction - 1 Wesley Smith, U. Wisconsin, January 21, 2014 Physics 301: Introduction - 1 Physics 301: Physics Today Prof. Wesley Smith, wsmith@hep.wisc.edu Undergraduate Physics Colloquium! Discussions of current research

More information

7 Physics at Hadron Colliders

7 Physics at Hadron Colliders 7 Physics at Hadron Colliders The present and future Hadron Colliders - The Tevatron and the LHC Test of the Standard Model at Hadron Colliders Jet, W/Z, Top-quark production Physics of Beauty Quarks (T.

More information

The Standard Model, Supersymmetry and ZooFinder at CDF. Matthew C. Cervantes Department of Physics Texas A&M University Master defense: 7/21/2006

The Standard Model, Supersymmetry and ZooFinder at CDF. Matthew C. Cervantes Department of Physics Texas A&M University Master defense: 7/21/2006 The Standard Model, Supersymmetry and ZooFinder at CDF Matthew C. Cervantes Department of Physics Texas A&M University Master defense: 7/21/2006 1 Outline The Standard Model of Particle Physics Supersymmetry

More information

4. The Standard Model

4. The Standard Model 4. The Standard Model Particle and Nuclear Physics Dr. Tina Potter Dr. Tina Potter 4. The Standard Model 1 In this section... Standard Model particle content Klein-Gordon equation Antimatter Interaction

More information

Particles and Strings Probing the Structure of Matter and Space-Time

Particles and Strings Probing the Structure of Matter and Space-Time Particles and Strings Probing the Structure of Matter and Space-Time University Hamburg DPG-Jahrestagung, Berlin, March 2005 2 Physics in the 20 th century Quantum Theory (QT) Planck, Bohr, Heisenberg,...

More information

Week 3 - Part 2 Recombination and Dark Matter. Joel Primack

Week 3 - Part 2 Recombination and Dark Matter. Joel Primack Astro/Phys 224 Spring 2012 Origin and Evolution of the Universe Week 3 - Part 2 Recombination and Dark Matter Joel Primack University of California, Santa Cruz http://pdg.lbl.gov/ In addition to the textbooks

More information

Particle physics today. Giulia Zanderighi (CERN & University of Oxford)

Particle physics today. Giulia Zanderighi (CERN & University of Oxford) Particle physics today Giulia Zanderighi (CERN & University of Oxford) Particle Physics Particle Physics is fundamental research, as opposed to many applied sciences (medicine, biology, chemistry, nano-science,

More information

SUSY Phenomenology & Experimental searches

SUSY Phenomenology & Experimental searches SUSY Phenomenology & Experimental searches Slides available at: Alex Tapper http://www.hep.ph.ic.ac.uk/~tapper/lecture.html Objectives - Know what Supersymmetry (SUSY) is - Understand qualitatively the

More information

Birth of electroweak theory from an Imperial perspective

Birth of electroweak theory from an Imperial perspective Birth of electroweak theory from an Imperial perspective Tom Kibble King s College London 2 Oct 2012 Electroweak theory Oct 2012 1 Outline Story of spontaneous symmetry breaking in gauge theories and electro-weak

More information

Review Chap. 18: Particle Physics

Review Chap. 18: Particle Physics Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material Review Chap. 18: Particle Physics Particles and fields: a new picture Quarks and leptons: the particle zoo

More information

New Physics below the Fermi Scale. Mikhail Shaposhnikov

New Physics below the Fermi Scale. Mikhail Shaposhnikov New Physics below the Fermi Scale Mikhail Shaposhnikov September 6, 2016 CERN, September 6, 2016 p. 1 The LHC has discovered something quite unexpected (at least, up to now, ICHEP 2016): The Higgs boson

More information

Nuclear and Particle Physics 3: Particle Physics. Lecture 1: Introduction to Particle Physics February 5th 2007

Nuclear and Particle Physics 3: Particle Physics. Lecture 1: Introduction to Particle Physics February 5th 2007 Nuclear and Particle Physics 3: Particle Physics Lecture 1: Introduction to Particle Physics February 5th 2007 Particle Physics (PP) a.k.a. High-Energy Physics (HEP) 1 Dr Victoria Martin JCMB room 4405

More information

Aharonov-Bohm Effect and Unification of Elementary Particles. Yutaka Hosotani, Osaka University Warsaw, May 2006

Aharonov-Bohm Effect and Unification of Elementary Particles. Yutaka Hosotani, Osaka University Warsaw, May 2006 Aharonov-Bohm Effect and Unification of Elementary Particles Yutaka Hosotani, Osaka University Warsaw, May 26 - Part 1 - Aharonov-Bohm effect Aharonov-Bohm Effect! B)! Fµν = (E, vs empty or vacuum!= Fµν

More information

Supersymmetry and other theories of Dark Matter Candidates

Supersymmetry and other theories of Dark Matter Candidates Supersymmetry and other theories of Dark Matter Candidates Ellie Lockner 798G Presentation 3/1/07 798G 3/1/07 1 Overview Why bother with a new theory? Why is Supersymmetry a good solution? Basics of Supersymmetry

More information

CHAPTER 14 Particle Physics

CHAPTER 14 Particle Physics CHAPTER 14 Particle Physics 14.1 Early Discoveries 14.2 The Fundamental Interactions 14.3 Classification of Particles 14.4 Conservation Laws and Symmetries 14.5 Quarks 14.6 The Families of Matter 14.7

More information

Elementary Particle Physics Glossary. Course organiser: Dr Marcella Bona February 9, 2016

Elementary Particle Physics Glossary. Course organiser: Dr Marcella Bona February 9, 2016 Elementary Particle Physics Glossary Course organiser: Dr Marcella Bona February 9, 2016 1 Contents 1 Terms A-C 5 1.1 Accelerator.............................. 5 1.2 Annihilation..............................

More information

Particle Physics. Dr Victoria Martin, Spring Semester 2012 Lecture 1: The Mysteries of Particle Physics, or Why should I take this course?

Particle Physics. Dr Victoria Martin, Spring Semester 2012 Lecture 1: The Mysteries of Particle Physics, or Why should I take this course? Particle Physics Dr Victoria Martin, Spring Semester 2012 Lecture 1: The Mysteries of Particle Physics, or Why should I take this course? Contents: Review of the Standard Model! What we know! What we don

More information

Astronomy, Astrophysics, and Cosmology

Astronomy, Astrophysics, and Cosmology Astronomy, Astrophysics, and Cosmology Luis A. Anchordoqui Department of Physics and Astronomy Lehman College, City University of New York Lesson IX April 12, 2016 arxiv:0706.1988 L. A. Anchordoqui (CUNY)

More information

Going beyond the Standard Model of Elementary Particle Physics

Going beyond the Standard Model of Elementary Particle Physics Going beyond the Standard Model of Elementary Particle Physics Saurabh D. Rindani PRL, Ahmedabad Symposium on Recent Trends in High Energy Physics November 19, 2011 77th Annual Meeting of the Indian Academy

More information

Astro-2: History of the Universe

Astro-2: History of the Universe Astro-2: History of the Universe Lecture 11; May 21 2013 Previously on astro-2 In an expanding universe the relationship between redshift and distance depends on the cosmological parameters (i.e. the geometry

More information

Higgs Field and Quantum Gravity

Higgs Field and Quantum Gravity Higgs Field and Quantum Gravity The magnetic induction creates a negative electric field, causing an electromagnetic inertia responsible for the relativistic mass change; it is the mysterious Higgs Field

More information

ALICE, ATLAS, CMS, LHCb, TOTEM, LHCf

ALICE, ATLAS, CMS, LHCb, TOTEM, LHCf LHC EXPERIMENTS LHC EXPERIMENTS ALICE, ATLAS, CMS, LHCb, TOTEM, LHCf ACE Antiproton Cell Experiment Antiprotons versus cancer cells Non LHC Experiments ASACUSA Atomic Spectroscopy And Collisions Using

More information

The Standard Model. 1 st 2 nd 3 rd Describes 3 of the 4 known fundamental forces. Separates particle into categories

The Standard Model. 1 st 2 nd 3 rd Describes 3 of the 4 known fundamental forces. Separates particle into categories The Standard Model 1 st 2 nd 3 rd Describes 3 of the 4 known fundamental forces. Separates particle into categories Bosons (force carriers) Photon, W, Z, gluon, Higgs Fermions (matter particles) 3 generations

More information

Supersymmetry and a Candidate for Dark Matter

Supersymmetry and a Candidate for Dark Matter Supersymmetry and a Candidate for Dark Matter Elizabeth Lockner Department of Physics, University of Maryland College Park, MD 20742 April 20, 2007. The Standard Model has been a powerful tool in understanding

More information

IX. Electroweak unification

IX. Electroweak unification IX. Electroweak unification The problem of divergence A theory of weak interactions only by means of W ± bosons leads to infinities e + e - γ W - W + e + W + ν e ν µ e - W - µ + µ Divergent integrals Figure

More information

A model of the basic interactions between elementary particles is defined by the following three ingredients:

A model of the basic interactions between elementary particles is defined by the following three ingredients: I. THE STANDARD MODEL A model of the basic interactions between elementary particles is defined by the following three ingredients:. The symmetries of the Lagrangian; 2. The representations of fermions

More information

Physics at the TeV Scale Discovery Prospects Using the ATLAS Detector at the LHC

Physics at the TeV Scale Discovery Prospects Using the ATLAS Detector at the LHC Physics at the TeV Scale Discovery Prospects Using the ATLAS Detector at the LHC Peter Krieger Carleton University Physics Motivations Experimental Theoretical New particles searches Standard Model Higgs

More information

String Theory in the LHC Era

String Theory in the LHC Era String Theory in the LHC Era J Marsano (marsano@uchicago.edu) 1 String Theory in the LHC Era 1. Electromagnetism and Special Relativity 2. The Quantum World 3. Why do we need the Higgs? 4. The Standard

More information

Discovery of the W and Z 0 Bosons

Discovery of the W and Z 0 Bosons Discovery of the W and Z 0 Bosons Status of the Standard Model ~1980 Planning the Search for W ± and Z 0 SppS, UA1 and UA2 The analyses and the observed events First measurements of W ± and Z 0 masses

More information

Introduction. Read: Ch 1 of M&S

Introduction. Read: Ch 1 of M&S Introduction What questions does this field address? Want to know the basic law of nature. Can we unify all the forces with one equation or one theory? Read: Ch 1 of M&S K.K. Gan L1: Introduction 1 Particle

More information

Par$cles. Ma#er is made of atoms. Atoms are made of leptons and quarks. Leptons. Quarks. atom nucleus nucleon quark m m m m

Par$cles. Ma#er is made of atoms. Atoms are made of leptons and quarks. Leptons. Quarks. atom nucleus nucleon quark m m m m Par$cles Ma#er is made of atoms atom nucleus nucleon quark 10-10 m 10-14 m 10-15 m 10-18 m Atoms are made of leptons and quarks Leptons ν e e Quarks u d What Have We Learned? Rela?vis?c Quantum Mechanics

More information

PH5211: High Energy Physics. Prafulla Kumar Behera Room: HSB-304B

PH5211: High Energy Physics. Prafulla Kumar Behera Room: HSB-304B PH5211: High Energy Physics Prafulla Kumar Behera E-mail:behera@iitm.ac.in Room: HSB-304B Information Class timing: Wed. 11am, Thur. 9am, Fri. 8am The course will be graded as follows: 1 st quiz (20 marks)

More information

The Matter-Antimatter Asymmetry and New Interactions

The Matter-Antimatter Asymmetry and New Interactions The Matter-Antimatter Asymmetry and New Interactions The baryon (matter) asymmetry The Sakharov conditions Possible mechanisms A new very weak interaction Recent Reviews M. Trodden, Electroweak baryogenesis,

More information